Alkali-free aluminoborosilicate glass and uses thereof

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Reexamination Certificate

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C501S064000, C501S067000, C501S069000, C501S070000

Reexamination Certificate

active

06329310

ABSTRACT:

FIELD OF THE INVENTION
The invention relates to an alkali-free aluminoborosilicate glass. The invention also relates to uses of this glass.
BACKGROUND OF THE INVENTION
High requirements are made of glasses for applications as substrates in liquid-crystal flat-panel display technology, for example in TN (twisted nematic)/STN (supertwisted nematic) displays, active matrix liquid crystal displays (AMLCDs), thin film transistors (TFTs) or plasma addressed liquid crystals (PALCs). Besides high thermal shock resistance and good resistance to the aggressive chemicals employed in the production process for flat-panel screens, the glasses should have high transparency over a broad spectral range (VIS, UV) and low density in order to save weight. Use as substrate material for integrated semiconductor circuits, for example in TFT displays (“chip on glass”) in addition requires thermal matching to the thin-film material a- or polysilicon (&agr;
20/300
=3.7×10
−6
/K) and the absence of alkali metal ions. Sodium oxide amounts resulting from production of more than 1500 ppm cannot be tolerated in view of the generally “poisoning” action due to diffusion of Na

into the semiconductor layer.
It should be possible to produce suitable glasses economically on a large industrial scale in adequate quality (no bubbles, knots, inclusions), for example in a float plant or by the drawing method. In particular, the production of thin. (<1 mm) streak-free substrates with low surface undulation by the drawing process requires high devitrification stability of the glasses. Compaction of the substrate during production, which has a disadvantageous effect on the semiconductor microstructure, can be countered by setting a suitable temperature-dependent viscosity characteristic line of the glass: with respect to thermal process and shape stability, it should have a high strain point (SP; temperature at a viscosity of 10
14.7
dPas), ideally above 700° C., or a high glass transition temperature T
g
, i.e. T
g
>720° C., while on the other hand not having excessively high melting and working (V
A
) points, i.e. a V
A
of ≦1330° C. Furthermore, a low density of the glasses is desired in order to keep the overall weight of the display low, in particular in the case of large screen formats.
The requirements of glass substrates for liquid crystal display (LCD) technology are also described in “Glass substrates for AMLCD applications: properties and implications” by J C Lapp, SPIE Proceedings, Vol. 3014, Invited paper (1997).
In principle, corresponding requirements are made of glasses for substrates in thin-film photovoltaics, especially based on microcrystalline silicon (&mgr;c-Si).
An essential prerequisite for the commercial success of thin-film photovoltaics against high-cost solar technology based on crystalline Si wafers is the presence of inexpensive high-temperature-resistant substrates.
At present, two different coating methods are known for the production of &mgr;c-Si solar cells. A process which has proven particularly favorable with respect to high deposition rates is a high-temperature chemical vapor deposition (CVD) process using inexpensive trichlorosilane as Si source. This process requires the heating of a suitable substrate to 1000° C. or above. The only suitable substrates are then comparatively expensive ceramics, graphite, silicon or similar materials. Use of transparent glass-ceramics has also been discussed in the literature (L. R. Pinckney: “Transparent, High Strain Point Glass-Ceramics”, Proc. 18th Intern. Conf. Glass, San Francisco; Amer. Ceram. Soc., Ohio, 1998, and L. R. Pinckney, G. H. Beall: “Nanocrystalline Non-Alkali Glass-Ceramics”, J. NonCryst. Solids 219 (1997)). Efficiencies achieved on small areas by the high temperature CVD process are currently about 11%.
As an alternative to the high-temperature approach, low temperature Si deposition processes have been developed which allow the use of the less expensive substrate material glass. One possibility here is the deposition of amorphous silicon at low temperatures of up to 300° C. and, in a subsequent step, the recrystallization of the layers using laser or zone-melting methods. In order to prevent deformation of the glass plate at the temperatures prevailing in the conditioning process, a special glass with very high heat resistance which is matched thermally to silicon is required. These glasses suitably have a glass transition temperature, Tof at least 750° C. As a consequence of the tendency to change over from a-Si to poly-Si coatings, the highest possible heat resistance of the substrate is also desired for substrates for TFT display technology.
The current development of &mgr;c-Si technology is moving in the direction of a substrate concept, i.e. the substrate material forms the basis of the solar cells and is opaque to the incident light. However, a development towards a less expensive superstrate arrangement (light passes through the substrate material, no cover glass necessary) is not excluded. In order to achieve high efficiencies, high transparency of the glass in the VIS/UV is then necessary, which means that the use of semi-transparent glass-ceramics, besides the above-mentioned cost reasons, proves to be disadvantageous.
The said requirement profile is satisfied most closely by alkaline earth metal aluminoborosilicate glasses. However, the known display or solar-cell substrate glasses described in the following specifications still have disadvantages and do not meet the entire range of requirements.
Numerous specifications describe glasses having relatively high B
2
O
3
contents, for example DE 196 01 922 A, JP 58-120 535 A, JP 60-141 642 A, JP 8-295 530 A, JP 9-169 538 A, JP 10-59 741 A, JP 10-722 37 A, EP 714 862 A1, EP 341 313 B1, and U.S. Pat. No. 5,374,595. These glasses do not have the requisite high glass transition temperatures or strain points.
The same applies to the low-SiO
2
glasses of JP 61-132 536 A and to the glasses of DE 197 39 912 Cl containing a maximum of 60% by weight of SiO
2
and at least 6.5% by weight of B
2
O
3
.
By contrast, B
2
O
3
-free glasses are described in U.S. Pat. No. 4,607,016, JP 1-126 239 A, JP 61-236 631 A and JP 61-261 232 A. Owing to the freedom from B
2
O
3
, the glasses have poor melting properties and tend toward devitrification. The glasses mentioned in WO 97/30001 likewise contain no B
2
O
3
.
DE 44 30 710 C1 describes borosilicate glasses having low boric acid contents and high SiO
2
contents (>75% by weight), which results in them having high viscosity even at high temperatures and means that they can only be melted and fined at high cost. In addition, these glasses, having glass transition temperatures T
g
of from 500 to 600° C., have only relatively low heat resistance.
DE 196 17 344 C1 and DE 196 03 698 C1 by the Applicant disclose alkali-free, tin-containing glasses having a coefficient of thermal expansion &agr;
20/300
of about 3.7-10
−6
/K and very good chemicals resistance. They are suitable for use in display technology. However, since they necessarily contain at least 1 or 2% by weight of the network modifier ZnO, they are not totally suitable, in particular for processing in a float plant.
Thus, the glasses of JP 61-295 256 A, which contain Pb and have a relatively high Zn content (≧3.5% by weight) are likewise not very suitable for the float process, since coatings of ZnO and PbO or Pb can easily form on the glass surface in the reducing forming gas atmosphere due to evaporation and subsequent condensation at an excessively high concentration.
JP 3-164 445 A describes glass-ceramics having ZnO contents of ≧5% by weight for displays and solar cells. They have the desired high glass transition temperatures, but are poorly matched to &mgr;c-Si with their thermal expansion of greater than 4.0·10
−6
/K.
Further glass-ceramics which have a relatively high Zn content (≧8% by weight) and in addition contain Pb are described in JP 1-208 343 A. These likewise have excessively high thermal expansion. Corre

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